JP3123136B2 - Surface emitting semiconductor laser, array thereof, surface emitting light emitting diode, array thereof and surface emitting pnpn device - Google Patents
Surface emitting semiconductor laser, array thereof, surface emitting light emitting diode, array thereof and surface emitting pnpn deviceInfo
- Publication number
- JP3123136B2 JP3123136B2 JP21252391A JP21252391A JP3123136B2 JP 3123136 B2 JP3123136 B2 JP 3123136B2 JP 21252391 A JP21252391 A JP 21252391A JP 21252391 A JP21252391 A JP 21252391A JP 3123136 B2 JP3123136 B2 JP 3123136B2
- Authority
- JP
- Japan
- Prior art keywords
- emitting
- substrate
- semiconductor laser
- array
- semiconductor
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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- 239000004065 semiconductor Substances 0.000 title claims description 65
- 239000000758 substrate Substances 0.000 claims description 46
- 230000010287 polarization Effects 0.000 description 35
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 15
- 238000005253 cladding Methods 0.000 description 9
- 238000004519 manufacturing process Methods 0.000 description 6
- 230000005684 electric field Effects 0.000 description 5
- 230000010355 oscillation Effects 0.000 description 5
- 229910004298 SiO 2 Inorganic materials 0.000 description 4
- 239000013078 crystal Substances 0.000 description 4
- 125000005842 heteroatom Chemical group 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 230000003287 optical effect Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 239000002019 doping agent Substances 0.000 description 3
- 239000002994 raw material Substances 0.000 description 3
- 238000001039 wet etching Methods 0.000 description 3
- RBFQJDQYXXHULB-UHFFFAOYSA-N arsane Chemical compound [AsH3] RBFQJDQYXXHULB-UHFFFAOYSA-N 0.000 description 2
- 238000003776 cleavage reaction Methods 0.000 description 2
- AXAZMDOAUQTMOW-UHFFFAOYSA-N dimethylzinc Chemical compound C[Zn]C AXAZMDOAUQTMOW-UHFFFAOYSA-N 0.000 description 2
- PZPGRFITIJYNEJ-UHFFFAOYSA-N disilane Chemical compound [SiH3][SiH3] PZPGRFITIJYNEJ-UHFFFAOYSA-N 0.000 description 2
- 238000001459 lithography Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 238000002488 metal-organic chemical vapour deposition Methods 0.000 description 2
- 238000000206 photolithography Methods 0.000 description 2
- 230000007017 scission Effects 0.000 description 2
- RGGPNXQUMRMPRA-UHFFFAOYSA-N triethylgallium Chemical compound CC[Ga](CC)CC RGGPNXQUMRMPRA-UHFFFAOYSA-N 0.000 description 2
- IBEFSUTVZWZJEL-UHFFFAOYSA-N trimethylindium Chemical compound C[In](C)C IBEFSUTVZWZJEL-UHFFFAOYSA-N 0.000 description 2
- 241001663154 Electron Species 0.000 description 1
- XYFCBTPGUUZFHI-UHFFFAOYSA-N Phosphine Chemical compound P XYFCBTPGUUZFHI-UHFFFAOYSA-N 0.000 description 1
- 238000002109 crystal growth method Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 239000000284 extract Substances 0.000 description 1
- 230000010365 information processing Effects 0.000 description 1
- 230000000737 periodic effect Effects 0.000 description 1
- 238000012827 research and development Methods 0.000 description 1
- 238000012552 review Methods 0.000 description 1
- 230000002269 spontaneous effect Effects 0.000 description 1
- JLTRXTDYQLMHGR-UHFFFAOYSA-N trimethylaluminium Chemical compound C[Al](C)C JLTRXTDYQLMHGR-UHFFFAOYSA-N 0.000 description 1
- XCZXGTMEAKBVPV-UHFFFAOYSA-N trimethylgallium Chemical compound C[Ga](C)C XCZXGTMEAKBVPV-UHFFFAOYSA-N 0.000 description 1
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- Semiconductor Lasers (AREA)
- Led Devices (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、偏波方向の制御性が良
くまた安定化された面発光型半導体レーザ及び個々の素
子の偏波方向が揃った半導体レーザアレー及び偏波方向
依存性のある発光ダイオード及び個々の素子の偏波方向
が揃った発光ダイオードアレーに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a surface-emitting type semiconductor laser in which the controllability of the polarization direction is good and stabilized, a semiconductor laser array in which the polarization directions of individual elements are aligned, and a polarization direction dependence. The present invention relates to a light emitting diode and a light emitting diode array in which polarization directions of individual elements are aligned.
【0002】[0002]
【従来の技術】近年、光ディスク用光源や光コンピュー
ティング応用など情報処理分野への応用として基板面に
対し垂直方向に光を取り出す面発光型半導体レーザの研
究開発が盛んに行われている。室温で連続動作する面発
光型半導体レーザもジャパニーズジャーナルオブアプラ
イドフィジックス誌(A.Ibarakiet al.
Jpn.J.Appl.Phys.Vol.28(19
89)L667頁)に報告されている。2. Description of the Related Art In recent years, research and development of a surface-emitting type semiconductor laser for extracting light in a direction perpendicular to a substrate surface has been actively performed as an application to an information processing field such as a light source for an optical disk and an optical computing application. Surface emitting semiconductor lasers that operate continuously at room temperature are also disclosed in Japanese Journal of Applied Physics (A. Ibaraki et al.
Jpn. J. Appl. Phys. Vol. 28 (19
89) L667).
【0003】通常の端面方向より光出力を取り出す半導
体レーザでは導波路構造により端面反射のモード選択性
が顕著であるため、安定にTEモードで発振する。面発
光型半導体レーザでも直線偏波で発振することがジャー
ナルオブクオンタムエレクトロニクス誌(K.Iga
et al.IEEE J.Quantum Elec
tron.Vol.QE−21(1985)663頁)
に報告され、その偏波方向は[110]方向または
[1,−1,0]方向で発信することがジャパニーズジ
ャーナルオブアプライドフィジックス誌(M.Shim
izu et al.Jpn.J.Appl.Phy
s.Vol.27(1989)1774頁)に報告され
ているが、面発光型半導体レーザではビーム垂直方向に
対し等方であるため偏波方向を一義的に定義することは
できず、また、不安定である場合もある。p側反射鏡で
ある誘電体多層膜の一方向側面にSiを蒸着し、損失を
設けることにより偏波方向を制御する試みもなされてい
る(平成3年春季応用物理学関係連合講演会講演予稿集
31a−D−2)。In a semiconductor laser that extracts light output from the normal end face direction, the mode selectivity of end face reflection is remarkable due to the waveguide structure, so that the semiconductor laser oscillates stably in the TE mode. Oscillation with linearly polarized light even in a surface-emitting type semiconductor laser is described in Journal of Quantum Electronics (K. Iga).
et al. IEEE J.I. Quantum Elec
tron. Vol. QE-21 (1985) p. 663)
It is reported that the polarization direction is transmitted in the [110] direction or the [1, -1, 0] direction, according to the Japanese Journal of Applied Physics (M. Shim).
Izu et al. Jpn. J. Appl. Phys
s. Vol. 27 (1989), p. 1774), but the surface-emitting type semiconductor laser is isotropic with respect to the beam vertical direction, so that the polarization direction cannot be uniquely defined and is unstable. In some cases. Attempts have been made to control the polarization direction by depositing Si on one side of the dielectric multilayer film, which is a p-side reflector, and providing a loss (Preliminary lecture of Spring 1991 Joint Lecture on Applied Physics). Vol. 31a-D-2).
【0004】また、通常の発光ダイオードでは偏波方向
依存性はなく、ランダムな電界ベクトルで発光してい
る。このため、偏波方向を制御するのはかなり困難であ
る。[0004] A normal light emitting diode has no polarization direction dependence and emits light with a random electric field vector. For this reason, it is quite difficult to control the polarization direction.
【0005】[0005]
【発明が解決しようとする課題】従来の面発光型半導体
レーザでは結晶表面の荒さやストレスによる非等方性、
ミラー面の非平行、メサ形状の非等方性、蒸着膜の非等
方性などの複合により偏波方向が決定するため、偏波方
向を制御し、安定化させることは困難であった。[11
0]方向または[1,−1,0]方向のどちらか一方に
損失を設け偏波方向を制御する方法では複雑な工程を必
要とし、また、ビーム形状が円形状より変形する可能性
もある。In the conventional surface-emitting type semiconductor laser, the anisotropy due to the roughness of the crystal surface and the stress,
Since the polarization direction is determined by the combination of the non-parallel mirror surface, the mesa shape anisotropy, and the anisotropy of the deposited film, it has been difficult to control and stabilize the polarization direction. [11
The method of controlling the polarization direction by providing a loss in either the [0] direction or the [1, -1, 0] direction requires a complicated process, and the beam shape may be deformed from a circular shape. .
【0006】また、従来の発光ダイオードでは放出光の
電界ベクトルはランダムであり、偏波方向は出射光の垂
直方向に対し依存性を持っていない。In the conventional light emitting diode, the electric field vector of the emitted light is random, and the polarization direction does not depend on the vertical direction of the emitted light.
【0007】さらに、偏波方向の制御されていない面発
光素子を同一基板上に集積化した面発光素子アレーでは
個々の素子の偏波方向が異なってしまう可能性が高く、
偏波方向がある一方向に揃った面発光素子アレーを提供
することは困難である。Further, in a surface emitting element array in which surface emitting elements whose polarization directions are not controlled are integrated on the same substrate, there is a high possibility that the polarization directions of individual elements are different.
It is difficult to provide a surface emitting element array in which the polarization direction is aligned in one direction.
【0008】本発明の目的は、活性層に偏波方向依存性
のある結晶を用いることにより、偏波方向の制御が容易
であり、素子のある一方向に損失を設けるなど複雑な製
造工程を必要としなく、ビーム形状を変形させる構造を
導入することのない面発光型半導体レーザ及び面発光型
発光ダイオード及びこの面発光型半導体レーザまたは面
発光型発光ダイオードを同一基板上に集積化した偏波方
向の揃った半導体レーザアレー及び発光ダイオードアレ
ーあるいは、面発光型pnpn素子を提供することにあ
る。An object of the present invention is to use a crystal having polarization direction dependency in the active layer, so that the polarization direction can be easily controlled and a complicated manufacturing process such as providing a loss in one direction of the element can be achieved. A surface-emitting semiconductor laser and a surface-emitting light-emitting diode that do not require and do not introduce a structure that deforms the beam shape, and a polarization in which the surface-emitting semiconductor laser or the surface-emitting light-emitting diode is integrated on the same substrate It is an object of the present invention to provide a semiconductor laser array and a light emitting diode array, or a surface emitting pnpn element, with aligned directions.
【0009】[0009]
【課題を解決するための手段】本発明の面発光型半導体
レーザは、半導体基板面方位が(001)面から[−
1,1,0]または[1,−1,0]方向に傾いた半導
体基板上に、自然超格子を形成した活性層を含む半導体
層を有し、該基板面に対し垂直方向に共振器を有するこ
とを特徴とする。According to the surface emitting semiconductor laser of the present invention, the semiconductor substrate has a [-] plane orientation of [-].
A semiconductor layer including an active layer having a natural superlattice formed on a semiconductor substrate inclined in the [1,1,0] or [1, -1,0] direction, and having a resonator perpendicular to the substrate surface; It is characterized by having.
【0010】また、本発明の半導体レーザアレーは、上
述の面発光型半導体レーザを同一基板上に集積化するこ
とを特徴とする。Further, a semiconductor laser array according to the present invention is characterized in that the above-mentioned surface-emitting type semiconductor laser is integrated on the same substrate.
【0011】本発明の面発光型発光ダイオードは、半導
体基板面方位が(001)面から[−1,1,0]また
は[1,−1,0]方向に傾いた半導体基板上に、自然
超格子を形成した活性層を含む半導体層を有し、該基板
表面または裏面より光を取り出す構造を有することを特
徴とする。The surface-emitting type light emitting diode of the present invention has a natural orientation on a semiconductor substrate whose plane orientation is inclined in the [-1,1,0] or [1, -1,0] direction from the (001) plane. The semiconductor device includes a semiconductor layer including an active layer in which a superlattice is formed, and has a structure in which light is extracted from the front surface or the back surface of the substrate.
【0012】さらに、本発明の発光ダイオードアレー
は、上述の面発光型発光ダイオードを同一基板上に集積
化することを特徴とする。Further, a light emitting diode array according to the present invention is characterized in that the above-mentioned surface emitting light emitting diodes are integrated on the same substrate.
【0013】また、面発光型pnpn素子の活性層に自
然超格子を有すること、あるいはそのアレーであること
を特徴とする。Further, the active layer of the surface emitting pnpn element has a natural superlattice or is an array thereof.
【0014】[0014]
【作用】GaInP,AlGaInPのエピタキシャル
成長層において[−1,1,1]または[1,−1,
1]方向に秩序性のある周期構造をもった自然超格子が
形成されていることが報告されている(例えば、アプラ
イドフィジックスレターズ誌(Gomyo et a
l.Appl.Phys.Lett.Vol.50(1
987)673頁))。また、自然超格子が形成された
半導体では、最低準位間の発光の電界ベクトルは自然超
格子の形成されている(−1,1,1)または(1,−
1,1)面内に偏っていることがフィジカルレビューレ
ターズ誌(A.Mascarenhas et al.
Phys.Rev.Lett.Vol.63(198
9)2108頁)に報告されている。In the GaInP or AlGaInP epitaxial growth layer, [-1,1,1] or [1, -1,
1] It has been reported that a natural superlattice having an ordered periodic structure is formed in the [1] direction (for example, Applied Physics Letters (Gomyo et a).
l. Appl. Phys. Lett. Vol. 50 (1
987) p. 673)). In a semiconductor in which a natural superlattice is formed, the electric field vector of light emission between the lowest levels is (-1, 1, 1) or (1,-) in which a natural superlattice is formed.
(1) The in-plane bias is due to the physical review letters (A. Mascarenhas et al.
Phys. Rev .. Lett. Vol. 63 (198
9) p. 2108).
【0015】本発明の面発光型半導体レーザは自然超格
子が形成されている活性層を有しており、光出力は基板
面に対し垂直方向に取り出されるため、例えば(00
1)面の基板を用いた場合、発振しきい値以下の自然放
出光の電界成分は[−1,1,0]方向に比べ、[11
0]方向が大きくなる。半導体レーザでは、利得の大き
い方向の偏波で発振するため、本発明の面発光型半導体
レーザは[110]方向の偏波で発信する。また、本発
明の面発光型発光ダイオードでは、[110]方向に偏
波した光の発光効率が高くなる。The surface-emitting type semiconductor laser of the present invention has an active layer in which a natural superlattice is formed, and an optical output is taken out in a direction perpendicular to the substrate surface.
When the substrate having the 1) plane is used, the electric field component of the spontaneous emission light equal to or lower than the oscillation threshold value is [11, 1, 0] compared to the [-1, 1, 0] direction.
0] direction increases. Since a semiconductor laser oscillates with a polarization in the direction of a large gain, the surface emitting semiconductor laser of the present invention emits with a polarization in the [110] direction. In the surface-emitting light emitting diode of the present invention, the luminous efficiency of light polarized in the [110] direction is increased.
【0016】また、基板結晶面方位が(001)面から
[−1,1,0]または[1,−1,0]方向に傾いた
半導体基板上に形成したエピタキシャル成長層では自然
超格子の秩序性が高くなり、4°から6°傾いた半導体
基板で最も強く自然超格子が形成される。この(00
1)面より傾きのある基板を用いることにより偏波選択
性がよりいっそう強くなり、面発光型半導体レーザでは
[110]方向の電界ベクトルをもった発光に効率よく
利得が与えられるため、発振しきい値電流の低減にもな
る。また面発光型発光ダイオードや面発光型pnpn素
子では[110]方向への偏波方向依存性がよりいっそ
う高くなる。In an epitaxially grown layer formed on a semiconductor substrate whose substrate crystal plane orientation is inclined in the [-1,1,0] or [1, -1,0] direction from the (001) plane, the order of the natural superlattice is obtained. And a natural superlattice is formed most strongly on a semiconductor substrate inclined from 4 ° to 6 °. This (00
1) The polarization selectivity is further enhanced by using a substrate inclined from the plane, and a surface-emitting type semiconductor laser can efficiently emit light having an electric field vector in the [110] direction, and thus can oscillate. It also reduces the threshold current. In the case of a surface emitting type light emitting diode or a surface emitting type pnpn element, the polarization direction dependence in the [110] direction is further increased.
【0017】さらに、本発明の面発光型半導体レーザま
たは面発光型発光ダイオードあるいはpnpn素子を同
一基板上に集積化した面発光素子アレーでは、個々の面
発光型素子の偏波方向を[110]方向に揃えることが
できる。Further, in the surface-emitting type semiconductor laser, the surface-emitting type light-emitting diode, or the pnpn element array of the present invention, the polarization direction of each surface-emitting type element is set to [110]. Can be aligned in any direction.
【0018】[0018]
【実施例】本発明の面発光型半導体レーザの一実施例を
図を用いて説明する。図1は本発明の面発光型半導体レ
ーザの断面図であり、図2にはその製造工程を説明する
ための図である。DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the surface emitting semiconductor laser according to the present invention will be described with reference to the drawings. FIG. 1 is a cross-sectional view of a surface-emitting type semiconductor laser of the present invention, and FIG. 2 is a view for explaining a manufacturing process thereof.
【0019】まず、図2(a)に示すように、n型Ga
As(001)基板1上に2.0μm厚のn型(Al
0 . 7 Ga0 . 3 )0 . 5 In0 . 5 Pクラッド層2、
2.0μm厚のアンドープGa0 . 5 In0 . 5 P活性
層3、1.0μm厚のp型(Al0 . 7 Ga0 . 3 )
0 . 5 In0 . 5 Pクラッド層4、20対のp型(Al
0. 1 Ga0 . 9 )0 . 5 In0 . 5 P/(Al0 . 7
Ga0 . 3 )0 . 5 In0. 5 P DBR多層膜5、
0.1μm厚のp型Ga0 . 5 In0 . 5 Pヘテロバッ
ファ層6、0.5μm厚のp型GaAsキャップ層7を
積層成長した。p型(Al0 . 1 Ga0 . 9 )0 . 5 I
n0 . 5 P/(Al0 . 7 Ga0 . 3 )0 . 5 In
0 . 5 P DBR多層膜5の層厚は発振波長に対してλ
/2周期になるようにした。結晶成長は減圧MOVPE
法を用いた。成長条件は、自然超格子が形成されるよう
に、温度660℃、圧力70Torr、V族原料供給量
/III族原料供給量比(V/III比)150とし
た。原料としては、トリメチルアルミニウム(TM
A)、トリエチルガリウム(TEG)、トリメチルイン
ジウム(TMI)、アルシン(AsH3 )、ホスフィン
(PH3 )、n型ドーパントとしてジシラン(Si2 H
6 )、p型ドーパントとしてジメチルジンク(DMZ)
を用いた。First, as shown in FIG.
An n-type (Al) having a thickness of 2.0 μm is formed on an As (001) substrate 1.
0. 7 Ga 0. 3) 0. 5 In 0. 5 P cladding layer 2,
2.0μm undoped Ga 0 thick. 5 In 0. 5 P active layer 3,1.0μm thickness of p-type (Al 0. 7 Ga 0. 3)
0. 5 In 0. 5 P cladding layer 4, 20 pairs of p-type (Al
0. 1 Ga 0. 9) 0 . 5 In 0. 5 P / (Al 0. 7
Ga 0. 3) 0. 5 In 0. 5 P DBR multi-layer film 5,
0.1μm thick p-type Ga 0. 5 In 0. 5 and the P hetero buffer layer 6,0.5Myuemu p-type GaAs cap layer 7 having a thickness laminated grow. p-type (Al 0. 1 Ga 0. 9) 0. 5 I
n 0. 5 P / (Al 0. 7 Ga 0. 3) 0. 5 In
0.5 The thickness of the P DBR multi-layer film 5 is λ with respect to the oscillation wavelength
/ 2 cycle. Crystal growth is under reduced pressure MOVPE
Method was used. The growth conditions were a temperature of 660 ° C., a pressure of 70 Torr, and a group V material supply amount / group III material supply amount ratio (V / III ratio) of 150 so as to form a natural superlattice. The raw material is trimethyl aluminum (TM
A), triethylgallium (TEG), trimethylindium (TMI), arsine (AsH 3 ), phosphine (PH 3 ), and disilane (Si 2 H) as an n-type dopant
6 ), dimethyl zinc (DMZ) as p-type dopant
Was used.
【0020】このウェハ上にリソグラフィ法により直径
7μmのSiO2 マスク12を形成した後、図2(b)
に示すように、p型(Al0 .7 Ga0 . 3 )0 . 5 I
n0. 5 Pクラッド層4が0.3μm程度残るように、
ウェットエッチングによりp型GaAsキャップ層7、
p型Ga0 . 5 In0 . 5 Pヘテロバッファ層6、p型
(Al0 . 1 Ga0 . 9 )0 . 5 In0 . 5 P/(Al
0 . 7 Ga0 . 3 )0. 5 In0 . 5 P DBR多層膜
5、p型(Al0 . 7 Ga0 .3 )0 . 5 In0 . 5 P
クラッド層4を除去した。After a 7 μm diameter SiO 2 mask 12 is formed on the wafer by lithography, FIG.
As shown in, p-type (Al 0 .7 Ga 0. 3 ) 0. 5 I
In order that the n 0.5 P cladding layer 4 remains about 0.3 μm,
P-type GaAs cap layer 7 by wet etching,
p-type Ga 0. 5 In 0. 5 P hetero buffer layer 6, p-type (Al 0. 1 Ga 0. 9) 0. 5 In 0. 5 P / (Al
0. 7 Ga 0. 3) 0. 5 In 0. 5 P DBR multi-layer film 5, p-type (Al 0. 7 Ga 0 .3 ) 0. 5 In 0. 5 P
The cladding layer 4 was removed.
【0021】つぎに、図2(c)に示すように、SiO
2 をマスクとして減圧MOVPE法により、3μm厚の
n型GaAsブロック層8を選択成長した。成長条件
は、温度650℃、圧力70Torr、V/III比4
5とした。原料としては、トリメチルガリウム(TM
G)、アルシン(AsH3 )、n型ドーパントとしてジ
シラン(Si2 H6 )、を用いた。n型GaAsブロッ
ク層8を成長後、SiO2 マスク12を除去する。Next, as shown in FIG.
Using the mask 2 as a mask, an n-type GaAs block layer 8 having a thickness of 3 μm was selectively grown by the reduced pressure MOVPE method. The growth conditions were as follows: temperature 650 ° C., pressure 70 Torr, V / III ratio 4
It was set to 5. As a raw material, trimethylgallium (TM
G), arsine (AsH 3 ), and disilane (Si 2 H 6 ) as an n-type dopant. After growing the n-type GaAs block layer 8, the SiO 2 mask 12 is removed.
【0022】つぎに、n電極10を形成し、図2(d)
に示すように、n電極上に塗布したレジスト13を、フ
ォトリソグラフィ法を用いてp側の円形メサが中心に位
置するように直径200μmの円形にパターニングした
後、このレジスト13をマスクとしてn電極10とn型
GaAs基板1をウェットエッチングにより除去し、光
出射用の窓とした。レジスト13を除去後、p電極11
を蒸着した。Next, an n-electrode 10 is formed, and FIG.
As shown in FIG. 5, after the resist 13 applied on the n-electrode is patterned by photolithography into a circle having a diameter of 200 μm so that the p-side circular mesa is located at the center, the resist 13 is used as a mask to form the n-electrode. 10 and the n-type GaAs substrate 1 were removed by wet etching to form a window for light emission. After removing the resist 13, the p-electrode 11
Was deposited.
【0023】図2(e)に示すようにn型GaAs基板
を取り除いたn型(Al0 . 7 Ga0 . 3 )0 . 5 In
0 . 5 Pクラッド層2上に誘電体多層膜反射鏡9を形成
した。この誘電体多層膜反射鏡9とp型(Al0 . 1 G
a0 . 9 )0 . 5 In0 . 5 P/(Al0 . 7 Ga
0 . 3 )0 . 5 In0 . 5P多層膜5で共振器を形成し
ている。最後に劈開により1つ1つの素子を分離し、p
電極側をヒートシンクに融着して実装した。[0023] n-type removal of the n-type GaAs substrate as shown in FIG. 2 (e) (Al 0. 7 Ga 0. 3) 0. 5 In
A dielectric multilayer mirror 9 was formed on the 0.5 P cladding layer 2. The dielectric multilayer reflector 9 and the p-type (Al 0.1 G
a 0. 9) 0. 5 In 0. 5 P / (Al 0. 7 Ga
0.3 ) The 0.5 In 0.5 P multilayer film 5 forms a resonator. Finally, each element is separated by cleavage, and p
The electrode side was mounted on a heat sink by fusing.
【0024】こうして得られた本実施例の面発光型半導
体レーザの発振時の偏波方向は[110]である。The thus obtained surface emitting semiconductor laser of this embodiment has a polarization direction of [110] at the time of oscillation.
【0025】基板面方位が(001)面から[−1,
1,0]方向に6°傾いたn型GaAs基板上に、図1
と同様の構造の面発光型半導体レーザを形成した。この
面発光型半導体レーザは、[110]方向に安定に偏波
しており、(001)基板を用いた面発光型半導体レー
ザに比べ、発振しきい値電流は15%低減された。The substrate plane orientation is shifted from the (001) plane by [-1,
1 on an n-type GaAs substrate tilted 6 ° in the [1,0] direction.
A surface-emitting type semiconductor laser having the same structure as described above was formed. This surface emitting semiconductor laser was stably polarized in the [110] direction, and the oscillation threshold current was reduced by 15% as compared with the surface emitting semiconductor laser using the (001) substrate.
【0026】図3に400μm間隔で9素子の面発光型
半導体レーザを同一基板上に集積した半導体レーザアレ
ーの構造を示す。各面発光型半導体レーザの構造は図1
と同様である。この半導体レーザアレーの個々のレーザ
ビームの偏波方向は[110]方向に揃っている。FIG. 3 shows a structure of a semiconductor laser array in which nine surface emitting semiconductor lasers are integrated on the same substrate at an interval of 400 μm. The structure of each surface emitting semiconductor laser is shown in FIG.
Is the same as The polarization directions of the individual laser beams of this semiconductor laser array are aligned in the [110] direction.
【0027】続いて、本発明の面発光型発光ダイオード
の一実施例を図を用いて説明する。図4は本発明の面発
光型発光ダイオードの断面図であり、図5はその製造工
程を示すための図である。Next, an embodiment of the surface emitting type light emitting diode of the present invention will be described with reference to the drawings. FIG. 4 is a cross-sectional view of the surface-emitting light emitting diode of the present invention, and FIG. 5 is a view showing a manufacturing process thereof.
【0028】まず、図5(a)に示すように、n型Ga
As(001)基板1上に2.0μm厚のn型(Al
0 . 7 Ga0 . 3 )0 . 5 In0 . 5 Pクラッド層2、
2.0μm厚のアンドープGa0 . 5 In0 . 5 P活性
層3、5.0μm厚のp型(Al0 . 7 Ga0 . 3 )
0 . 5 In0 . 5 Pクラッド層4、0.1μm厚のp型
Ga0 . 5 In0 . 5 Pヘテロバッファ層6、0.5μ
m厚のp型GaAsキャップ層7を積層成長した。結晶
成長法、成長条件、原料は上述の面発光型半導体レーザ
と同一である。図5(b)に示すように、このウェハ上
にリソグラフィ法により直径30μmの穴を開けたSi
O2 絶縁膜12を形成した。First, as shown in FIG.
An n-type (Al) having a thickness of 2.0 μm is formed on an As (001) substrate 1.
0. 7 Ga 0. 3) 0. 5 In 0. 5 P cladding layer 2,
2.0μm undoped Ga 0 thick. 5 In 0. 5 P active layer 3,5.0μm thickness of p-type (Al 0. 7 Ga 0. 3)
0. 5 In 0. 5 P cladding layer 4,0.1Myuemu p-type Ga 0 thick. 5 In 0. 5 P hetero buffer layer 6,0.5μ
An m-thick p-type GaAs cap layer 7 was stacked and grown. The crystal growth method, growth conditions, and raw materials are the same as those of the above-described surface-emitting type semiconductor laser. As shown in FIG. 5 (b), a 30 μm-diameter hole was formed on this wafer by lithography.
An O 2 insulating film 12 was formed.
【0029】つぎに、n電極10を形成し、図2(c)
に示すように、n電極上に塗布したレジスト13を、フ
ォトリソグラフィ法を用いてp側のSiO2絶縁膜12
の円形の穴が中心に位置するように直径200μmの円
形にパターニングした後、このレジスト13をマスクと
してn電極10とn型GaAs基板1をウェットエッチ
ングにより除去し、光出射用の窓とした。図2(d)に
示すように、レジストを除去後、p電極11を蒸着し
た。最後に劈開により1つ1つの素子を分離し、p電極
側をヒートシンクに融着して実装した。Next, an n-electrode 10 is formed, and FIG.
As shown in FIG. 3, a resist 13 applied on an n-electrode is coated with a p-side SiO 2 insulating film 12 by photolithography.
Then, the n-electrode 10 and the n-type GaAs substrate 1 were removed by wet etching using the resist 13 as a mask to form a window for light emission. As shown in FIG. 2D, after removing the resist, a p-electrode 11 was deposited. Finally, each element was separated by cleavage, and the p-electrode side was mounted on a heat sink by fusing.
【0030】こうして得られた本発明の面発光型発光ダ
イオードは偏波方向依存性が高く放出光の65%以上が
[110]方向に偏光している。The surface emitting light emitting diode of the present invention thus obtained has a high polarization direction dependency, and 65% or more of the emitted light is polarized in the [110] direction.
【0031】基板面方位が(001)面から[−1,
1,0]方向に6°傾いたn型GaAs基板上に、図4
と同様の構造の面発光型発光ダイオードを形成した。こ
の面発光型発光ダイオードでは(001)基板を用いた
面発光型発光ダイオードに比べ、さらに偏波方向依存性
が高く放出光の75%以上が[110]方向に偏光して
いる。The substrate plane orientation is shifted from the (001) plane by [-1,
4 on an n-type GaAs substrate tilted 6 ° in the [1,0] direction.
A surface-emitting light emitting diode having the same structure as that of Example 1 was formed. In this surface-emitting light emitting diode, the polarization direction dependence is higher and 75% or more of the emitted light is polarized in the [110] direction as compared with the surface-emitting light-emitting diode using the (001) substrate.
【0032】図6には400μm間隔で9素子の面発光
型発光ダイオードを同一基板上に集積した発光ダイオー
ドアレーの構造を示す。各面発光型発光ダイオードの構
造は図4と同様である。この発光ダイオードアレーの個
々の放出光の偏波方向は[110]方向に揃っている。FIG. 6 shows the structure of a light emitting diode array in which nine surface emitting light emitting diodes are integrated on the same substrate at 400 μm intervals. The structure of each surface-emitting light emitting diode is the same as that of FIG. The polarization direction of each emitted light of this light emitting diode array is aligned in the [110] direction.
【0033】また変発明の面発光型pnpn素子の一実
施例として、n型GaAs基板上に、n−(Alx Ga
1 - x )0 . 5 In0 . 5 P(0<x<1)、P−(A
lY Ga1 - Y )0 . 5 In0 . 5 P(0<Y<x<
1)、アンドープGa0 . 5 In0 . 5 P活性層、n−
(AlY Ga1 - Y )0 . 5 In0 . 5 P、p−(Al
x Ga1 - x )0 . 5 In0 . 5 P、p−GaAsから
なる半導体層を形成し、前述の面発光型発光ダイオード
と同様に電極を形成し、実装した。このpnpn素子で
も偏波方向依存性の高い発光が得られた。この素子はス
イッチング素子や光機能素子として応用できる。またア
レーにすると、偏波方向のそろったpnpn素子アレー
が、均一良く得られる。As one embodiment of the surface-emitting type pnpn device of the invention, n- (Al x Ga.sub.x) is formed on an n-type GaAs substrate.
1-x ) 0.5 In 0.5 P (0 <x <1), P- (A
l Y Ga 1 -.. Y ) 0 5 In 0 5 P (0 <Y <x <
1), an undoped Ga 0. 5 In 0. 5 P active layer, n-
.. (Al Y Ga 1 - Y) 0 5 In 0 5 P, p- (Al
x Ga 1 -.. x) 0 5 In 0 5 P, to form a semiconductor layer made of p-GaAs, to form an electrode in the same manner as described above for the surface-emitting light-emitting diodes, it mounted. Even with this pnpn element, light emission highly dependent on the polarization direction was obtained. This element can be applied as a switching element or an optical function element. When an array is used, a pnpn element array having a uniform polarization direction can be obtained with good uniformity.
【0034】[0034]
【発明の効果】本発明の面発光型半導体レーザでは、安
定な偏波方向の制御が可能であり、一方向に損失を設け
るなど複雑な製造工程を必要としないため、少ない工程
で製作できる。従って、信頼性の高い偏波面制御型の面
発光型半導体レーザができる。According to the surface emitting semiconductor laser of the present invention, the polarization direction can be controlled stably and a complicated manufacturing process such as providing a loss in one direction is not required. Therefore, a highly reliable polarization-controlled surface emitting semiconductor laser can be obtained.
【0035】また、本発明の面発光型発光ダイオードで
は、偏波方向依存性があり、その方向の制御が可能であ
る。Further, the surface emitting type light emitting diode of the present invention has polarization direction dependency, and the direction can be controlled.
【0036】また、これらの素子を同一基板上に集積化
した半導体レーザアレー及び発光ダイオードアレーで
は、集積した全ての素子の偏波方向を一方向に揃えるこ
とが可能である。In a semiconductor laser array and a light emitting diode array in which these elements are integrated on the same substrate, the polarization directions of all the integrated elements can be aligned in one direction.
【図1】本発明の面発光型半導体レーザの一実施例の断
面図である。FIG. 1 is a sectional view of one embodiment of a surface emitting semiconductor laser according to the present invention.
【図2】本発明の面発光型半導体レーザの製造工程を説
明するための図である。FIG. 2 is a diagram for explaining a manufacturing process of the surface-emitting type semiconductor laser of the present invention.
【図3】本発明の半導体レーザアレーの一実施例の構造
図である。FIG. 3 is a structural diagram of one embodiment of a semiconductor laser array of the present invention.
【図4】本発明の面発光型発光ダイオードの一実施例の
断面図である。FIG. 4 is a cross-sectional view of one embodiment of the surface emitting light emitting diode of the present invention.
【図5】本発明の面発光型発光ダイオードの製造工程を
説明するための図である。FIG. 5 is a diagram for explaining a manufacturing process of the surface-emitting light emitting diode of the present invention.
【図6】本発明の一実施例の発光ダイオードアレーの構
造図である。FIG. 6 is a structural view of a light emitting diode array according to one embodiment of the present invention.
1 n型GaAs基板 2 n型(Al0 . 7 Ga0 . 3 )0 . 5 In0 . 5 P
クラッド層 3 アンドープGa0 . 5 In0 . 5 P活性層 4 p型(Al0 . 7 Ga0 . 3 )0 . 5 In0 . 5 P
クラッド層 5 p型(Al0 . 1 Ga0 . 9 )0 . 5 In0 . 5 P
/(Al0 . 7 Ga0 . 3 )0 . 5 In0 . 5 P DBR多層膜 6 p型Ga0 . 5 In0 . 5 Pヘテロバッファ層 7 p型GaAsキャップ層 8 n型GaAsブロック層 9 誘電体多層膜反射鏡 10 n電極 11 p電極 12 SiO2 絶縁膜 13 レジスト1 n-type GaAs substrate 2 n-type (Al 0. 7 Ga 0. 3) 0. 5 In 0. 5 P
Cladding layer 3 undoped Ga 0. 5 In 0. 5 P active layer 4 p-type (Al 0. 7 Ga 0. 3) 0. 5 In 0. 5 P
Cladding layer 5 p-type (Al 0. 1 Ga 0. 9) 0. 5 In 0. 5 P
/ (Al 0. 7 Ga 0 . 3) 0. 5 In 0. 5 P DBR multi-layer film 6 p-type Ga 0. 5 In 0. 5 P hetero buffer layer 7 p-type GaAs cap layer 8 n-type GaAs block layer 9 Dielectric multilayer film reflector 10 n-electrode 11 p-electrode 12 SiO 2 insulating film 13 resist
フロントページの続き (56)参考文献 特開 平3−104292(JP,A) 特開 平3−159289(JP,A) 特開 平4−199589(JP,A) 特開 平4−259263(JP,A) 特開 平4−273490(JP,A) 特開 平4−340288(JP,A) IEEE J.Quantum El ectron.24[9](1988)p. 1845−1855 (58)調査した分野(Int.Cl.7,DB名) H01S 5/00 - 5/50 H01L 33/00 Continuation of front page (56) References JP-A-3-104292 (JP, A) JP-A-3-159289 (JP, A) JP-A-4-199589 (JP, A) JP-A-4-259263 (JP) , A) JP-A-4-273490 (JP, A) JP-A-4-340288 (JP, A) IEEE J.I. Quantum Electron. 24 [9] (1988) p. 1845-1855 (58) Fields investigated (Int. Cl. 7 , DB name) H01S 5/00-5/50 H01L 33/00
Claims (7)
[−1,1,0]または[1,−1,0]方向に傾いた
半導体基板上に、自然超格子を形成した活性層を含む半
導体層を有し、該基板面に対し垂直方向に共振器を有す
ることを特徴とする面発光型半導体レーザ。An active layer having a natural superlattice formed on a semiconductor substrate having a semiconductor substrate plane orientation inclined in a [-1,1,0] or [1, -1,0] direction from a (001) plane. A surface-emitting type semiconductor laser comprising: a semiconductor layer including a semiconductor layer; and a resonator in a direction perpendicular to the substrate surface.
[−1,1,0]または[1,−1,0]方向に傾いた
半導体基板上に、自然超格子を形成した活性層を含む半
導体層を有し、該基板面に対し垂直方向に共振器を有す
る面発光型半導体レーザを同一基板上に一括して集積化
したことを特徴とする面発光型半導体レーザアレー。2. The semiconductor substrate has a plane orientation from a (001) plane.
A semiconductor layer including an active layer having a natural superlattice formed on a semiconductor substrate inclined in the [-1,1,0] or [1, -1,0] direction ; integrated collectively on the same substrate surface-emitting type semiconductor lasers having a cavity in a vertical direction against
Surface-emitting type semiconductor laser array, characterized in that the.
同一基板上に集積化したことを特徴とする面発光型半導
体レーザアレー。3. A surface-emitting type semiconductor laser array, wherein the surface-emitting type semiconductor laser according to claim 1 is integrated on the same substrate.
[−1,1,0]または[1,−1,0]方向に傾いた
半導体基板上に、自然超格子を形成した活性層を含む半
導体層を有し、該基板表面または裏面より光を取り出す
構造を有することを特徴とする面発光型発光ダイオー
ド。4. An active layer in which a natural superlattice is formed on a semiconductor substrate whose plane orientation is inclined in the [-1,1,0] or [1, -1,0] direction from a (001) plane. A surface-emitting light emitting diode, comprising: a semiconductor layer including a light emitting layer; and a structure for extracting light from the front surface or the back surface of the substrate.
を同一基板上に集積化したことを特徴とする面発光型発
光ダイオードアレー。5. A surface emitting light emitting diode array, wherein the surface emitting light emitting diodes according to claim 4 are integrated on the same substrate.
[−1,1,0]または[1,−1,0]方向に傾いた
半導体基板上に、自然超格子を形成した活性層とpnp
n構造の半導体を含み、基板表面または裏面から光を取
り出す構造を有することを特徴とする面発光型pnpn
素子。6. The semiconductor substrate has a plane orientation from a (001) plane.
An active layer having a natural superlattice formed on a semiconductor substrate inclined in the [-1,1,0] or [1, -1,0] direction and a pnp
A surface-emitting pnpn including a semiconductor having an n-type structure and having a structure for extracting light from a front surface or a back surface of the substrate.
element.
同一基板上に集積化したことを特徴とする面発光型pn
pn素子アレー。7. A surface-emitting type pn device wherein the surface-emitting type pnpn element according to claim 6 is integrated on the same substrate.
pn element array.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP21252391A JP3123136B2 (en) | 1991-08-26 | 1991-08-26 | Surface emitting semiconductor laser, array thereof, surface emitting light emitting diode, array thereof and surface emitting pnpn device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP21252391A JP3123136B2 (en) | 1991-08-26 | 1991-08-26 | Surface emitting semiconductor laser, array thereof, surface emitting light emitting diode, array thereof and surface emitting pnpn device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0555704A JPH0555704A (en) | 1993-03-05 |
| JP3123136B2 true JP3123136B2 (en) | 2001-01-09 |
Family
ID=16624084
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP21252391A Expired - Fee Related JP3123136B2 (en) | 1991-08-26 | 1991-08-26 | Surface emitting semiconductor laser, array thereof, surface emitting light emitting diode, array thereof and surface emitting pnpn device |
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| Country | Link |
|---|---|
| JP (1) | JP3123136B2 (en) |
Families Citing this family (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH08242037A (en) * | 1995-03-03 | 1996-09-17 | Nec Corp | Planar semiconductor light emitting element |
| JP4010095B2 (en) * | 1999-10-01 | 2007-11-21 | 富士ゼロックス株式会社 | Surface emitting semiconductor laser and laser array |
| US6967985B2 (en) | 2002-02-12 | 2005-11-22 | Sanyo Electric Co., Ltd. | Surface emission semiconductor laser device |
| JP3843245B2 (en) * | 2002-06-26 | 2006-11-08 | 宣彦 澤木 | Semiconductor light emitting element and semiconductor light emitting device |
| DE10234976B4 (en) * | 2002-07-31 | 2012-05-03 | Osram Opto Semiconductors Gmbh | Surface emitting semiconductor laser chip and method for its production |
| KR100590775B1 (en) * | 2004-12-08 | 2006-06-19 | 한국전자통신연구원 | Silicon-based light emitting diode |
| JP2008028139A (en) * | 2006-07-21 | 2008-02-07 | Ricoh Co Ltd | Semiconductor chip manufacturing method, surface emitting semiconductor laser, surface emitting semiconductor laser array, optical scanning device, and image forming apparatus |
| CN114024211B (en) * | 2021-12-13 | 2024-12-31 | 长春中科长光时空光电技术有限公司 | Semiconductor device and method for manufacturing the same |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0734496B2 (en) * | 1989-09-19 | 1995-04-12 | 三菱電機株式会社 | Semiconductor laser |
| JPH03159289A (en) * | 1989-11-17 | 1991-07-09 | Fujitsu Ltd | Manufacture of semiconductor laser |
| JPH04199589A (en) * | 1990-11-28 | 1992-07-20 | Mitsubishi Electric Corp | Visible light plane emission laser device |
| JP2931678B2 (en) * | 1991-02-14 | 1999-08-09 | 株式会社東芝 | Semiconductor light emitting device |
-
1991
- 1991-08-26 JP JP21252391A patent/JP3123136B2/en not_active Expired - Fee Related
Non-Patent Citations (1)
| Title |
|---|
| IEEE J.Quantum Electron.24[9](1988)p.1845−1855 |
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|---|---|
| JPH0555704A (en) | 1993-03-05 |
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